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Introduction to Symmetrical Components

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Protection Basics:
Introduction to Symmetrical Components
1. Introduction
Symmetrical components is the name given to a methodology,
which was discovered in 1913 by Charles Legeyt Fortescue
who later presented a paper on his findings entitled, “Method of
Symmetrical Co-ordinates Applied to the Solution of Polyphase
Networks.” Fortescue demonstrated that any set of unbalanced
three-phase quantities could be expressed as the sum of three
symmetrical sets of balanced phasors. Using this tool, unbalanced
system conditions, like those caused by common fault types may
be visualized and analyzed. Additionally, most microprocessorbased relays operate from symmetrical component quantities
and so the importance of a good understanding of this tool is
self-evident.
2. Positive, Negative and Zero Sequence
Components
According to Fortescue’s methodology, there are three sets of
independent components in a three-phase system: positive,
negative and zero for both current and voltage. Positive sequence
voltages (Figure 1) are supplied by generators within the system
and are always present. A second set of balanced phasors are
also equal in magnitude and displaced 120 degrees apart, but
display a counter-clockwise rotation sequence of A-C-B (Figure 2),
which represents a negative sequence. The final set of balanced
phasors is equal in magnitude and in phase with each other,
however since there is no rotation sequence (Figure 3) this is
known as a zero sequence.
Figure 3.
Zero Sequence Components
3. Introduction to Symmetrical
Components
The symmetrical components can be used to determine any
unbalanced current or voltage (Ia, Ib, Ic or Va, Vb, Vc which
reference unbalanced line-to-neutral phasors) as follows:
Ia = I1 + I2 + I0
Va = V1 + V2 + V0
Ib = a2I1 + aI2 + I0
Vb = a2V1 + aV2 + V0
Ic = aI1 + a2I2 + I0
Vc = aV1 + a2V2 + V0
The sequence currents or voltages from a three-phase unbalanced
set can be calculated using the following equations:
Zero Sequence Component:
I0 = ⅓ (Ia + Ib + Ic) V0 = ⅓ (Va + Vb + Vc)
Positive Sequence Component:
I1 = ⅓ (Ia + aIb + a2Ic)
V1 = ⅓ (Va + aVb + a2Vc)
Negative Sequence Component:
I2 = ⅓ (Ia + a2Ib + aIc) V2 = ⅓ (Va + a2Vb + aVc)
The independence of the symmetrical components and their
resultant summation follow the principle of superposition, which
is the basis for its practical usage in protective relaying.
Figure 1.
Positive Sequence Components;
A-B-C
Figure 2.
Negative Sequence Components;
A-C-B
Before proceeding further, a mathematical explanation of the “a”
operator is required. Within Fortescue’s formulas, the “a” operator
shifts a vector by an angle of 120 degrees counter-clockwise,
and the “a2” operator performs a 240 degrees counter-clockwise
phase shift. According to Fortescue, a balanced system will have
only positive sequence currents and voltages. For example, as
Protection Basics: Introduction to Symmetrical Components
79
shown in Figure 4, the calculation of symmetrical components
in a three-phase balanced or symmetrical system results in only
positive sequence voltages, 3V1. Similarly, the currents also have
equal magnitudes and phase angles of 120 degrees apart, which
would produce a result of only positive sequence and no negative
or zero sequence currents for a balanced system.
For unbalanced systems, such as an open-phase there will be
positive, negative and possibly zero-sequence currents. Referring
to the open-phase example in Figure 5, it can be seen that the
calculation of the symmetrical components results in positive,
negative and zero sequence currents of 3I1, 3I2, and 3I0. However,
since the voltages are balanced in magnitude and phase angle,
the result would be the same as the balanced system in Figure 4,
which produces only positive sequence voltage.
5. References
[1] J. L. Blackburn, T. J. Domin, 2007, “Protective Relaying, Principles
and Applications, Third Edition,” Taylor & Francis Group, LLC, Boca
Raton, FL, pp.75-80
[2] GE Publication, “Fundamentals of Modern Protective Relaying,”
Instruction Manual, Markham, Ontario, 2007
Similarly for a single phase to ground fault as shown in Figure 6,
there will be positive, negative and zero sequence currents (3I1, 3I2,
and 3I0) and voltages (3V1, 3V2, and 3V0).
4. Summary
Under a no fault condition, the power system is considered to
be essentially a symmetrical system and therefore only positive
sequence currents and voltages exist. At the time of a fault,
positive, negative and possibly zero sequence currents and
voltages exist. Using real world phase voltages and currents
along with Fortescue’s formulas, all positive, negative and zero
sequence currents can be calculated. Protective relays use these
sequence components along with phase current and/or voltage
data as the input to protective elements.
Figure 5.
Open-Phase Unbalanced / Non-Symmetrical System
Figure 4.
Three-Phase Balanced / Symmetrical System
Figure 6.
Single Phase-Ground Fault Unbalanced / Non-Symmetrical System
80
Protection Basics: Introduction to Symmetrical Components
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